math.exp on complex, real part

Percentage Accurate: 100.0% → 100.0%
Time: 3.4s
Alternatives: 7
Speedup: 1.0×

Specification

?
\[e^{re} \cdot \cos im \]
(FPCore (re im)
  :precision binary64
  (* (exp re) (cos im)))
double code(double re, double im) {
	return exp(re) * cos(im);
}
module fmin_fmax_functions
    implicit none
    private
    public fmax
    public fmin

    interface fmax
        module procedure fmax88
        module procedure fmax44
        module procedure fmax84
        module procedure fmax48
    end interface
    interface fmin
        module procedure fmin88
        module procedure fmin44
        module procedure fmin84
        module procedure fmin48
    end interface
contains
    real(8) function fmax88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(4) function fmax44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(8) function fmax84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmax48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
    end function
    real(8) function fmin88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(4) function fmin44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(8) function fmin84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmin48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
    end function
end module

real(8) function code(re, im)
use fmin_fmax_functions
    real(8), intent (in) :: re
    real(8), intent (in) :: im
    code = exp(re) * cos(im)
end function
public static double code(double re, double im) {
	return Math.exp(re) * Math.cos(im);
}
def code(re, im):
	return math.exp(re) * math.cos(im)
function code(re, im)
	return Float64(exp(re) * cos(im))
end
function tmp = code(re, im)
	tmp = exp(re) * cos(im);
end
code[re_, im_] := N[(N[Exp[re], $MachinePrecision] * N[Cos[im], $MachinePrecision]), $MachinePrecision]
e^{re} \cdot \cos im

Local Percentage Accuracy vs ?

The average percentage accuracy by input value. Horizontal axis shows value of an input variable; the variable is choosen in the title. Vertical axis is accuracy; higher is better. Red represent the original program, while blue represents Herbie's suggestion. These can be toggled with buttons below the plot. The line is an average while dots represent individual samples.

Accuracy vs Speed?

Herbie found 7 alternatives:

AlternativeAccuracySpeedup
The accuracy (vertical axis) and speed (horizontal axis) of each alternatives. Up and to the right is better. The red square shows the initial program, and each blue circle shows an alternative.The line shows the best available speed-accuracy tradeoffs.

Initial Program: 100.0% accurate, 1.0× speedup?

\[e^{re} \cdot \cos im \]
(FPCore (re im)
  :precision binary64
  (* (exp re) (cos im)))
double code(double re, double im) {
	return exp(re) * cos(im);
}
module fmin_fmax_functions
    implicit none
    private
    public fmax
    public fmin

    interface fmax
        module procedure fmax88
        module procedure fmax44
        module procedure fmax84
        module procedure fmax48
    end interface
    interface fmin
        module procedure fmin88
        module procedure fmin44
        module procedure fmin84
        module procedure fmin48
    end interface
contains
    real(8) function fmax88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(4) function fmax44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(8) function fmax84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmax48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
    end function
    real(8) function fmin88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(4) function fmin44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(8) function fmin84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmin48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
    end function
end module

real(8) function code(re, im)
use fmin_fmax_functions
    real(8), intent (in) :: re
    real(8), intent (in) :: im
    code = exp(re) * cos(im)
end function
public static double code(double re, double im) {
	return Math.exp(re) * Math.cos(im);
}
def code(re, im):
	return math.exp(re) * math.cos(im)
function code(re, im)
	return Float64(exp(re) * cos(im))
end
function tmp = code(re, im)
	tmp = exp(re) * cos(im);
end
code[re_, im_] := N[(N[Exp[re], $MachinePrecision] * N[Cos[im], $MachinePrecision]), $MachinePrecision]
e^{re} \cdot \cos im

Alternative 1: 99.0% accurate, 0.2× speedup?

\[\begin{array}{l} t_0 := \left(1 + re\right) \cdot \cos im\\ t_1 := e^{re} \cdot \cos im\\ \mathbf{if}\;t\_1 \leq -\infty:\\ \;\;\;\;e^{re} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right)\\ \mathbf{elif}\;t\_1 \leq -0.02:\\ \;\;\;\;t\_0\\ \mathbf{elif}\;t\_1 \leq 4 \cdot 10^{-137}:\\ \;\;\;\;e^{re}\\ \mathbf{elif}\;t\_1 \leq 0.9999558625966923:\\ \;\;\;\;t\_0\\ \mathbf{else}:\\ \;\;\;\;e^{re}\\ \end{array} \]
(FPCore (re im)
  :precision binary64
  (let* ((t_0 (* (+ 1.0 re) (cos im))) (t_1 (* (exp re) (cos im))))
  (if (<= t_1 (- INFINITY))
    (* (exp re) (fma (* im im) -0.5 1.0))
    (if (<= t_1 -0.02)
      t_0
      (if (<= t_1 4e-137)
        (exp re)
        (if (<= t_1 0.9999558625966923) t_0 (exp re)))))))
double code(double re, double im) {
	double t_0 = (1.0 + re) * cos(im);
	double t_1 = exp(re) * cos(im);
	double tmp;
	if (t_1 <= -((double) INFINITY)) {
		tmp = exp(re) * fma((im * im), -0.5, 1.0);
	} else if (t_1 <= -0.02) {
		tmp = t_0;
	} else if (t_1 <= 4e-137) {
		tmp = exp(re);
	} else if (t_1 <= 0.9999558625966923) {
		tmp = t_0;
	} else {
		tmp = exp(re);
	}
	return tmp;
}
function code(re, im)
	t_0 = Float64(Float64(1.0 + re) * cos(im))
	t_1 = Float64(exp(re) * cos(im))
	tmp = 0.0
	if (t_1 <= Float64(-Inf))
		tmp = Float64(exp(re) * fma(Float64(im * im), -0.5, 1.0));
	elseif (t_1 <= -0.02)
		tmp = t_0;
	elseif (t_1 <= 4e-137)
		tmp = exp(re);
	elseif (t_1 <= 0.9999558625966923)
		tmp = t_0;
	else
		tmp = exp(re);
	end
	return tmp
end
code[re_, im_] := Block[{t$95$0 = N[(N[(1.0 + re), $MachinePrecision] * N[Cos[im], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[(N[Exp[re], $MachinePrecision] * N[Cos[im], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t$95$1, (-Infinity)], N[(N[Exp[re], $MachinePrecision] * N[(N[(im * im), $MachinePrecision] * -0.5 + 1.0), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$1, -0.02], t$95$0, If[LessEqual[t$95$1, 4e-137], N[Exp[re], $MachinePrecision], If[LessEqual[t$95$1, 0.9999558625966923], t$95$0, N[Exp[re], $MachinePrecision]]]]]]]
\begin{array}{l}
t_0 := \left(1 + re\right) \cdot \cos im\\
t_1 := e^{re} \cdot \cos im\\
\mathbf{if}\;t\_1 \leq -\infty:\\
\;\;\;\;e^{re} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right)\\

\mathbf{elif}\;t\_1 \leq -0.02:\\
\;\;\;\;t\_0\\

\mathbf{elif}\;t\_1 \leq 4 \cdot 10^{-137}:\\
\;\;\;\;e^{re}\\

\mathbf{elif}\;t\_1 \leq 0.9999558625966923:\\
\;\;\;\;t\_0\\

\mathbf{else}:\\
\;\;\;\;e^{re}\\


\end{array}
Derivation
  1. Split input into 3 regimes
  2. if (*.f64 (exp.f64 re) (cos.f64 im)) < -inf.0

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in im around 0

      \[\leadsto e^{re} \cdot \color{blue}{\left(1 + \frac{-1}{2} \cdot {im}^{2}\right)} \]
    3. Step-by-step derivation
      1. lower-+.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}}\right) \]
      2. lower-*.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}}\right) \]
      3. lower-pow.f6462.0%

        \[\leadsto e^{re} \cdot \left(1 + -0.5 \cdot {im}^{\color{blue}{2}}\right) \]
    4. Applied rewrites62.0%

      \[\leadsto e^{re} \cdot \color{blue}{\left(1 + -0.5 \cdot {im}^{2}\right)} \]
    5. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}}\right) \]
      2. +-commutativeN/A

        \[\leadsto e^{re} \cdot \left(\frac{-1}{2} \cdot {im}^{2} + \color{blue}{1}\right) \]
      3. lift-*.f64N/A

        \[\leadsto e^{re} \cdot \left(\frac{-1}{2} \cdot {im}^{2} + 1\right) \]
      4. *-commutativeN/A

        \[\leadsto e^{re} \cdot \left({im}^{2} \cdot \frac{-1}{2} + 1\right) \]
      5. lower-fma.f6462.0%

        \[\leadsto e^{re} \cdot \mathsf{fma}\left({im}^{2}, \color{blue}{-0.5}, 1\right) \]
      6. lift-pow.f64N/A

        \[\leadsto e^{re} \cdot \mathsf{fma}\left({im}^{2}, \frac{-1}{2}, 1\right) \]
      7. unpow2N/A

        \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, \frac{-1}{2}, 1\right) \]
      8. lower-*.f6462.0%

        \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    6. Applied rewrites62.0%

      \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, \color{blue}{-0.5}, 1\right) \]

    if -inf.0 < (*.f64 (exp.f64 re) (cos.f64 im)) < -0.02 or 3.9999999999999999e-137 < (*.f64 (exp.f64 re) (cos.f64 im)) < 0.99995586259669234

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in re around 0

      \[\leadsto \color{blue}{\left(1 + re\right)} \cdot \cos im \]
    3. Step-by-step derivation
      1. lower-+.f6452.1%

        \[\leadsto \left(1 + \color{blue}{re}\right) \cdot \cos im \]
    4. Applied rewrites52.1%

      \[\leadsto \color{blue}{\left(1 + re\right)} \cdot \cos im \]

    if -0.02 < (*.f64 (exp.f64 re) (cos.f64 im)) < 3.9999999999999999e-137 or 0.99995586259669234 < (*.f64 (exp.f64 re) (cos.f64 im))

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in re around 0

      \[\leadsto \color{blue}{\cos im} \]
    3. Step-by-step derivation
      1. lower-cos.f6451.2%

        \[\leadsto \cos im \]
    4. Applied rewrites51.2%

      \[\leadsto \color{blue}{\cos im} \]
    5. Taylor expanded in im around 0

      \[\leadsto 1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}} \]
    6. Step-by-step derivation
      1. lower-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lower-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. lower-pow.f6428.7%

        \[\leadsto 1 + -0.5 \cdot {im}^{2} \]
    7. Applied rewrites28.7%

      \[\leadsto 1 + \color{blue}{-0.5 \cdot {im}^{2}} \]
    8. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lift-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. *-commutativeN/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      4. lift-pow.f64N/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      5. pow2N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      6. lift-*.f64N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      7. +-commutativeN/A

        \[\leadsto \left(im \cdot im\right) \cdot \frac{-1}{2} + 1 \]
      8. lift-fma.f6428.7%

        \[\leadsto \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    9. Applied rewrites28.7%

      \[\leadsto \color{blue}{\mathsf{fma}\left(im \cdot im, -0.5, 1\right)} \]
    10. Taylor expanded in im around 0

      \[\leadsto \color{blue}{e^{re}} \]
    11. Step-by-step derivation
      1. lower-exp.f6470.0%

        \[\leadsto e^{re} \]
    12. Applied rewrites70.0%

      \[\leadsto \color{blue}{e^{re}} \]
  3. Recombined 3 regimes into one program.
  4. Add Preprocessing

Alternative 2: 98.7% accurate, 0.2× speedup?

\[\begin{array}{l} t_0 := e^{re} \cdot \cos im\\ \mathbf{if}\;t\_0 \leq -\infty:\\ \;\;\;\;e^{re} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right)\\ \mathbf{elif}\;t\_0 \leq -0.02:\\ \;\;\;\;\cos im\\ \mathbf{elif}\;t\_0 \leq 4 \cdot 10^{-137}:\\ \;\;\;\;e^{re}\\ \mathbf{elif}\;t\_0 \leq 0.9999558625966923:\\ \;\;\;\;\cos im\\ \mathbf{else}:\\ \;\;\;\;e^{re}\\ \end{array} \]
(FPCore (re im)
  :precision binary64
  (let* ((t_0 (* (exp re) (cos im))))
  (if (<= t_0 (- INFINITY))
    (* (exp re) (fma (* im im) -0.5 1.0))
    (if (<= t_0 -0.02)
      (cos im)
      (if (<= t_0 4e-137)
        (exp re)
        (if (<= t_0 0.9999558625966923) (cos im) (exp re)))))))
double code(double re, double im) {
	double t_0 = exp(re) * cos(im);
	double tmp;
	if (t_0 <= -((double) INFINITY)) {
		tmp = exp(re) * fma((im * im), -0.5, 1.0);
	} else if (t_0 <= -0.02) {
		tmp = cos(im);
	} else if (t_0 <= 4e-137) {
		tmp = exp(re);
	} else if (t_0 <= 0.9999558625966923) {
		tmp = cos(im);
	} else {
		tmp = exp(re);
	}
	return tmp;
}
function code(re, im)
	t_0 = Float64(exp(re) * cos(im))
	tmp = 0.0
	if (t_0 <= Float64(-Inf))
		tmp = Float64(exp(re) * fma(Float64(im * im), -0.5, 1.0));
	elseif (t_0 <= -0.02)
		tmp = cos(im);
	elseif (t_0 <= 4e-137)
		tmp = exp(re);
	elseif (t_0 <= 0.9999558625966923)
		tmp = cos(im);
	else
		tmp = exp(re);
	end
	return tmp
end
code[re_, im_] := Block[{t$95$0 = N[(N[Exp[re], $MachinePrecision] * N[Cos[im], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[t$95$0, (-Infinity)], N[(N[Exp[re], $MachinePrecision] * N[(N[(im * im), $MachinePrecision] * -0.5 + 1.0), $MachinePrecision]), $MachinePrecision], If[LessEqual[t$95$0, -0.02], N[Cos[im], $MachinePrecision], If[LessEqual[t$95$0, 4e-137], N[Exp[re], $MachinePrecision], If[LessEqual[t$95$0, 0.9999558625966923], N[Cos[im], $MachinePrecision], N[Exp[re], $MachinePrecision]]]]]]
\begin{array}{l}
t_0 := e^{re} \cdot \cos im\\
\mathbf{if}\;t\_0 \leq -\infty:\\
\;\;\;\;e^{re} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right)\\

\mathbf{elif}\;t\_0 \leq -0.02:\\
\;\;\;\;\cos im\\

\mathbf{elif}\;t\_0 \leq 4 \cdot 10^{-137}:\\
\;\;\;\;e^{re}\\

\mathbf{elif}\;t\_0 \leq 0.9999558625966923:\\
\;\;\;\;\cos im\\

\mathbf{else}:\\
\;\;\;\;e^{re}\\


\end{array}
Derivation
  1. Split input into 3 regimes
  2. if (*.f64 (exp.f64 re) (cos.f64 im)) < -inf.0

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in im around 0

      \[\leadsto e^{re} \cdot \color{blue}{\left(1 + \frac{-1}{2} \cdot {im}^{2}\right)} \]
    3. Step-by-step derivation
      1. lower-+.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}}\right) \]
      2. lower-*.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}}\right) \]
      3. lower-pow.f6462.0%

        \[\leadsto e^{re} \cdot \left(1 + -0.5 \cdot {im}^{\color{blue}{2}}\right) \]
    4. Applied rewrites62.0%

      \[\leadsto e^{re} \cdot \color{blue}{\left(1 + -0.5 \cdot {im}^{2}\right)} \]
    5. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}}\right) \]
      2. +-commutativeN/A

        \[\leadsto e^{re} \cdot \left(\frac{-1}{2} \cdot {im}^{2} + \color{blue}{1}\right) \]
      3. lift-*.f64N/A

        \[\leadsto e^{re} \cdot \left(\frac{-1}{2} \cdot {im}^{2} + 1\right) \]
      4. *-commutativeN/A

        \[\leadsto e^{re} \cdot \left({im}^{2} \cdot \frac{-1}{2} + 1\right) \]
      5. lower-fma.f6462.0%

        \[\leadsto e^{re} \cdot \mathsf{fma}\left({im}^{2}, \color{blue}{-0.5}, 1\right) \]
      6. lift-pow.f64N/A

        \[\leadsto e^{re} \cdot \mathsf{fma}\left({im}^{2}, \frac{-1}{2}, 1\right) \]
      7. unpow2N/A

        \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, \frac{-1}{2}, 1\right) \]
      8. lower-*.f6462.0%

        \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    6. Applied rewrites62.0%

      \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, \color{blue}{-0.5}, 1\right) \]

    if -inf.0 < (*.f64 (exp.f64 re) (cos.f64 im)) < -0.02 or 3.9999999999999999e-137 < (*.f64 (exp.f64 re) (cos.f64 im)) < 0.99995586259669234

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in re around 0

      \[\leadsto \color{blue}{\cos im} \]
    3. Step-by-step derivation
      1. lower-cos.f6451.2%

        \[\leadsto \cos im \]
    4. Applied rewrites51.2%

      \[\leadsto \color{blue}{\cos im} \]

    if -0.02 < (*.f64 (exp.f64 re) (cos.f64 im)) < 3.9999999999999999e-137 or 0.99995586259669234 < (*.f64 (exp.f64 re) (cos.f64 im))

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in re around 0

      \[\leadsto \color{blue}{\cos im} \]
    3. Step-by-step derivation
      1. lower-cos.f6451.2%

        \[\leadsto \cos im \]
    4. Applied rewrites51.2%

      \[\leadsto \color{blue}{\cos im} \]
    5. Taylor expanded in im around 0

      \[\leadsto 1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}} \]
    6. Step-by-step derivation
      1. lower-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lower-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. lower-pow.f6428.7%

        \[\leadsto 1 + -0.5 \cdot {im}^{2} \]
    7. Applied rewrites28.7%

      \[\leadsto 1 + \color{blue}{-0.5 \cdot {im}^{2}} \]
    8. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lift-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. *-commutativeN/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      4. lift-pow.f64N/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      5. pow2N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      6. lift-*.f64N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      7. +-commutativeN/A

        \[\leadsto \left(im \cdot im\right) \cdot \frac{-1}{2} + 1 \]
      8. lift-fma.f6428.7%

        \[\leadsto \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    9. Applied rewrites28.7%

      \[\leadsto \color{blue}{\mathsf{fma}\left(im \cdot im, -0.5, 1\right)} \]
    10. Taylor expanded in im around 0

      \[\leadsto \color{blue}{e^{re}} \]
    11. Step-by-step derivation
      1. lower-exp.f6470.0%

        \[\leadsto e^{re} \]
    12. Applied rewrites70.0%

      \[\leadsto \color{blue}{e^{re}} \]
  3. Recombined 3 regimes into one program.
  4. Add Preprocessing

Alternative 3: 76.6% accurate, 0.7× speedup?

\[\begin{array}{l} \mathbf{if}\;e^{re} \cdot \cos im \leq -0.02:\\ \;\;\;\;e^{re} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right)\\ \mathbf{else}:\\ \;\;\;\;e^{re}\\ \end{array} \]
(FPCore (re im)
  :precision binary64
  (if (<= (* (exp re) (cos im)) -0.02)
  (* (exp re) (fma (* im im) -0.5 1.0))
  (exp re)))
double code(double re, double im) {
	double tmp;
	if ((exp(re) * cos(im)) <= -0.02) {
		tmp = exp(re) * fma((im * im), -0.5, 1.0);
	} else {
		tmp = exp(re);
	}
	return tmp;
}
function code(re, im)
	tmp = 0.0
	if (Float64(exp(re) * cos(im)) <= -0.02)
		tmp = Float64(exp(re) * fma(Float64(im * im), -0.5, 1.0));
	else
		tmp = exp(re);
	end
	return tmp
end
code[re_, im_] := If[LessEqual[N[(N[Exp[re], $MachinePrecision] * N[Cos[im], $MachinePrecision]), $MachinePrecision], -0.02], N[(N[Exp[re], $MachinePrecision] * N[(N[(im * im), $MachinePrecision] * -0.5 + 1.0), $MachinePrecision]), $MachinePrecision], N[Exp[re], $MachinePrecision]]
\begin{array}{l}
\mathbf{if}\;e^{re} \cdot \cos im \leq -0.02:\\
\;\;\;\;e^{re} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right)\\

\mathbf{else}:\\
\;\;\;\;e^{re}\\


\end{array}
Derivation
  1. Split input into 2 regimes
  2. if (*.f64 (exp.f64 re) (cos.f64 im)) < -0.02

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in im around 0

      \[\leadsto e^{re} \cdot \color{blue}{\left(1 + \frac{-1}{2} \cdot {im}^{2}\right)} \]
    3. Step-by-step derivation
      1. lower-+.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}}\right) \]
      2. lower-*.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}}\right) \]
      3. lower-pow.f6462.0%

        \[\leadsto e^{re} \cdot \left(1 + -0.5 \cdot {im}^{\color{blue}{2}}\right) \]
    4. Applied rewrites62.0%

      \[\leadsto e^{re} \cdot \color{blue}{\left(1 + -0.5 \cdot {im}^{2}\right)} \]
    5. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}}\right) \]
      2. +-commutativeN/A

        \[\leadsto e^{re} \cdot \left(\frac{-1}{2} \cdot {im}^{2} + \color{blue}{1}\right) \]
      3. lift-*.f64N/A

        \[\leadsto e^{re} \cdot \left(\frac{-1}{2} \cdot {im}^{2} + 1\right) \]
      4. *-commutativeN/A

        \[\leadsto e^{re} \cdot \left({im}^{2} \cdot \frac{-1}{2} + 1\right) \]
      5. lower-fma.f6462.0%

        \[\leadsto e^{re} \cdot \mathsf{fma}\left({im}^{2}, \color{blue}{-0.5}, 1\right) \]
      6. lift-pow.f64N/A

        \[\leadsto e^{re} \cdot \mathsf{fma}\left({im}^{2}, \frac{-1}{2}, 1\right) \]
      7. unpow2N/A

        \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, \frac{-1}{2}, 1\right) \]
      8. lower-*.f6462.0%

        \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    6. Applied rewrites62.0%

      \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, \color{blue}{-0.5}, 1\right) \]

    if -0.02 < (*.f64 (exp.f64 re) (cos.f64 im))

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in re around 0

      \[\leadsto \color{blue}{\cos im} \]
    3. Step-by-step derivation
      1. lower-cos.f6451.2%

        \[\leadsto \cos im \]
    4. Applied rewrites51.2%

      \[\leadsto \color{blue}{\cos im} \]
    5. Taylor expanded in im around 0

      \[\leadsto 1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}} \]
    6. Step-by-step derivation
      1. lower-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lower-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. lower-pow.f6428.7%

        \[\leadsto 1 + -0.5 \cdot {im}^{2} \]
    7. Applied rewrites28.7%

      \[\leadsto 1 + \color{blue}{-0.5 \cdot {im}^{2}} \]
    8. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lift-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. *-commutativeN/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      4. lift-pow.f64N/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      5. pow2N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      6. lift-*.f64N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      7. +-commutativeN/A

        \[\leadsto \left(im \cdot im\right) \cdot \frac{-1}{2} + 1 \]
      8. lift-fma.f6428.7%

        \[\leadsto \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    9. Applied rewrites28.7%

      \[\leadsto \color{blue}{\mathsf{fma}\left(im \cdot im, -0.5, 1\right)} \]
    10. Taylor expanded in im around 0

      \[\leadsto \color{blue}{e^{re}} \]
    11. Step-by-step derivation
      1. lower-exp.f6470.0%

        \[\leadsto e^{re} \]
    12. Applied rewrites70.0%

      \[\leadsto \color{blue}{e^{re}} \]
  3. Recombined 2 regimes into one program.
  4. Add Preprocessing

Alternative 4: 75.3% accurate, 0.7× speedup?

\[\begin{array}{l} \mathbf{if}\;e^{re} \cdot \cos im \leq -0.02:\\ \;\;\;\;\left(1 + re\right) \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right)\\ \mathbf{else}:\\ \;\;\;\;e^{re}\\ \end{array} \]
(FPCore (re im)
  :precision binary64
  (if (<= (* (exp re) (cos im)) -0.02)
  (* (+ 1.0 re) (fma (* im im) -0.5 1.0))
  (exp re)))
double code(double re, double im) {
	double tmp;
	if ((exp(re) * cos(im)) <= -0.02) {
		tmp = (1.0 + re) * fma((im * im), -0.5, 1.0);
	} else {
		tmp = exp(re);
	}
	return tmp;
}
function code(re, im)
	tmp = 0.0
	if (Float64(exp(re) * cos(im)) <= -0.02)
		tmp = Float64(Float64(1.0 + re) * fma(Float64(im * im), -0.5, 1.0));
	else
		tmp = exp(re);
	end
	return tmp
end
code[re_, im_] := If[LessEqual[N[(N[Exp[re], $MachinePrecision] * N[Cos[im], $MachinePrecision]), $MachinePrecision], -0.02], N[(N[(1.0 + re), $MachinePrecision] * N[(N[(im * im), $MachinePrecision] * -0.5 + 1.0), $MachinePrecision]), $MachinePrecision], N[Exp[re], $MachinePrecision]]
\begin{array}{l}
\mathbf{if}\;e^{re} \cdot \cos im \leq -0.02:\\
\;\;\;\;\left(1 + re\right) \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right)\\

\mathbf{else}:\\
\;\;\;\;e^{re}\\


\end{array}
Derivation
  1. Split input into 2 regimes
  2. if (*.f64 (exp.f64 re) (cos.f64 im)) < -0.02

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in im around 0

      \[\leadsto e^{re} \cdot \color{blue}{\left(1 + \frac{-1}{2} \cdot {im}^{2}\right)} \]
    3. Step-by-step derivation
      1. lower-+.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}}\right) \]
      2. lower-*.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}}\right) \]
      3. lower-pow.f6462.0%

        \[\leadsto e^{re} \cdot \left(1 + -0.5 \cdot {im}^{\color{blue}{2}}\right) \]
    4. Applied rewrites62.0%

      \[\leadsto e^{re} \cdot \color{blue}{\left(1 + -0.5 \cdot {im}^{2}\right)} \]
    5. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto e^{re} \cdot \left(1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}}\right) \]
      2. +-commutativeN/A

        \[\leadsto e^{re} \cdot \left(\frac{-1}{2} \cdot {im}^{2} + \color{blue}{1}\right) \]
      3. lift-*.f64N/A

        \[\leadsto e^{re} \cdot \left(\frac{-1}{2} \cdot {im}^{2} + 1\right) \]
      4. *-commutativeN/A

        \[\leadsto e^{re} \cdot \left({im}^{2} \cdot \frac{-1}{2} + 1\right) \]
      5. lower-fma.f6462.0%

        \[\leadsto e^{re} \cdot \mathsf{fma}\left({im}^{2}, \color{blue}{-0.5}, 1\right) \]
      6. lift-pow.f64N/A

        \[\leadsto e^{re} \cdot \mathsf{fma}\left({im}^{2}, \frac{-1}{2}, 1\right) \]
      7. unpow2N/A

        \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, \frac{-1}{2}, 1\right) \]
      8. lower-*.f6462.0%

        \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    6. Applied rewrites62.0%

      \[\leadsto e^{re} \cdot \mathsf{fma}\left(im \cdot im, \color{blue}{-0.5}, 1\right) \]
    7. Taylor expanded in re around 0

      \[\leadsto \color{blue}{\left(1 + re\right)} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    8. Step-by-step derivation
      1. lower-+.f6430.8%

        \[\leadsto \left(1 + \color{blue}{re}\right) \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    9. Applied rewrites30.8%

      \[\leadsto \color{blue}{\left(1 + re\right)} \cdot \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]

    if -0.02 < (*.f64 (exp.f64 re) (cos.f64 im))

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in re around 0

      \[\leadsto \color{blue}{\cos im} \]
    3. Step-by-step derivation
      1. lower-cos.f6451.2%

        \[\leadsto \cos im \]
    4. Applied rewrites51.2%

      \[\leadsto \color{blue}{\cos im} \]
    5. Taylor expanded in im around 0

      \[\leadsto 1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}} \]
    6. Step-by-step derivation
      1. lower-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lower-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. lower-pow.f6428.7%

        \[\leadsto 1 + -0.5 \cdot {im}^{2} \]
    7. Applied rewrites28.7%

      \[\leadsto 1 + \color{blue}{-0.5 \cdot {im}^{2}} \]
    8. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lift-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. *-commutativeN/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      4. lift-pow.f64N/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      5. pow2N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      6. lift-*.f64N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      7. +-commutativeN/A

        \[\leadsto \left(im \cdot im\right) \cdot \frac{-1}{2} + 1 \]
      8. lift-fma.f6428.7%

        \[\leadsto \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    9. Applied rewrites28.7%

      \[\leadsto \color{blue}{\mathsf{fma}\left(im \cdot im, -0.5, 1\right)} \]
    10. Taylor expanded in im around 0

      \[\leadsto \color{blue}{e^{re}} \]
    11. Step-by-step derivation
      1. lower-exp.f6470.0%

        \[\leadsto e^{re} \]
    12. Applied rewrites70.0%

      \[\leadsto \color{blue}{e^{re}} \]
  3. Recombined 2 regimes into one program.
  4. Add Preprocessing

Alternative 5: 73.7% accurate, 0.8× speedup?

\[\begin{array}{l} \mathbf{if}\;e^{re} \cdot \cos im \leq -0.02:\\ \;\;\;\;\mathsf{fma}\left(im \cdot im, -0.5, 1\right)\\ \mathbf{else}:\\ \;\;\;\;e^{re}\\ \end{array} \]
(FPCore (re im)
  :precision binary64
  (if (<= (* (exp re) (cos im)) -0.02)
  (fma (* im im) -0.5 1.0)
  (exp re)))
double code(double re, double im) {
	double tmp;
	if ((exp(re) * cos(im)) <= -0.02) {
		tmp = fma((im * im), -0.5, 1.0);
	} else {
		tmp = exp(re);
	}
	return tmp;
}
function code(re, im)
	tmp = 0.0
	if (Float64(exp(re) * cos(im)) <= -0.02)
		tmp = fma(Float64(im * im), -0.5, 1.0);
	else
		tmp = exp(re);
	end
	return tmp
end
code[re_, im_] := If[LessEqual[N[(N[Exp[re], $MachinePrecision] * N[Cos[im], $MachinePrecision]), $MachinePrecision], -0.02], N[(N[(im * im), $MachinePrecision] * -0.5 + 1.0), $MachinePrecision], N[Exp[re], $MachinePrecision]]
\begin{array}{l}
\mathbf{if}\;e^{re} \cdot \cos im \leq -0.02:\\
\;\;\;\;\mathsf{fma}\left(im \cdot im, -0.5, 1\right)\\

\mathbf{else}:\\
\;\;\;\;e^{re}\\


\end{array}
Derivation
  1. Split input into 2 regimes
  2. if (*.f64 (exp.f64 re) (cos.f64 im)) < -0.02

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in re around 0

      \[\leadsto \color{blue}{\cos im} \]
    3. Step-by-step derivation
      1. lower-cos.f6451.2%

        \[\leadsto \cos im \]
    4. Applied rewrites51.2%

      \[\leadsto \color{blue}{\cos im} \]
    5. Taylor expanded in im around 0

      \[\leadsto 1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}} \]
    6. Step-by-step derivation
      1. lower-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lower-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. lower-pow.f6428.7%

        \[\leadsto 1 + -0.5 \cdot {im}^{2} \]
    7. Applied rewrites28.7%

      \[\leadsto 1 + \color{blue}{-0.5 \cdot {im}^{2}} \]
    8. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lift-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. *-commutativeN/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      4. lift-pow.f64N/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      5. pow2N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      6. lift-*.f64N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      7. +-commutativeN/A

        \[\leadsto \left(im \cdot im\right) \cdot \frac{-1}{2} + 1 \]
      8. lift-fma.f6428.7%

        \[\leadsto \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    9. Applied rewrites28.7%

      \[\leadsto \color{blue}{\mathsf{fma}\left(im \cdot im, -0.5, 1\right)} \]

    if -0.02 < (*.f64 (exp.f64 re) (cos.f64 im))

    1. Initial program 100.0%

      \[e^{re} \cdot \cos im \]
    2. Taylor expanded in re around 0

      \[\leadsto \color{blue}{\cos im} \]
    3. Step-by-step derivation
      1. lower-cos.f6451.2%

        \[\leadsto \cos im \]
    4. Applied rewrites51.2%

      \[\leadsto \color{blue}{\cos im} \]
    5. Taylor expanded in im around 0

      \[\leadsto 1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}} \]
    6. Step-by-step derivation
      1. lower-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lower-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. lower-pow.f6428.7%

        \[\leadsto 1 + -0.5 \cdot {im}^{2} \]
    7. Applied rewrites28.7%

      \[\leadsto 1 + \color{blue}{-0.5 \cdot {im}^{2}} \]
    8. Step-by-step derivation
      1. lift-+.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
      2. lift-*.f64N/A

        \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
      3. *-commutativeN/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      4. lift-pow.f64N/A

        \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
      5. pow2N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      6. lift-*.f64N/A

        \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
      7. +-commutativeN/A

        \[\leadsto \left(im \cdot im\right) \cdot \frac{-1}{2} + 1 \]
      8. lift-fma.f6428.7%

        \[\leadsto \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
    9. Applied rewrites28.7%

      \[\leadsto \color{blue}{\mathsf{fma}\left(im \cdot im, -0.5, 1\right)} \]
    10. Taylor expanded in im around 0

      \[\leadsto \color{blue}{e^{re}} \]
    11. Step-by-step derivation
      1. lower-exp.f6470.0%

        \[\leadsto e^{re} \]
    12. Applied rewrites70.0%

      \[\leadsto \color{blue}{e^{re}} \]
  3. Recombined 2 regimes into one program.
  4. Add Preprocessing

Alternative 6: 28.7% accurate, 5.4× speedup?

\[\mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
(FPCore (re im)
  :precision binary64
  (fma (* im im) -0.5 1.0))
double code(double re, double im) {
	return fma((im * im), -0.5, 1.0);
}
function code(re, im)
	return fma(Float64(im * im), -0.5, 1.0)
end
code[re_, im_] := N[(N[(im * im), $MachinePrecision] * -0.5 + 1.0), $MachinePrecision]
\mathsf{fma}\left(im \cdot im, -0.5, 1\right)
Derivation
  1. Initial program 100.0%

    \[e^{re} \cdot \cos im \]
  2. Taylor expanded in re around 0

    \[\leadsto \color{blue}{\cos im} \]
  3. Step-by-step derivation
    1. lower-cos.f6451.2%

      \[\leadsto \cos im \]
  4. Applied rewrites51.2%

    \[\leadsto \color{blue}{\cos im} \]
  5. Taylor expanded in im around 0

    \[\leadsto 1 + \color{blue}{\frac{-1}{2} \cdot {im}^{2}} \]
  6. Step-by-step derivation
    1. lower-+.f64N/A

      \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
    2. lower-*.f64N/A

      \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
    3. lower-pow.f6428.7%

      \[\leadsto 1 + -0.5 \cdot {im}^{2} \]
  7. Applied rewrites28.7%

    \[\leadsto 1 + \color{blue}{-0.5 \cdot {im}^{2}} \]
  8. Step-by-step derivation
    1. lift-+.f64N/A

      \[\leadsto 1 + \frac{-1}{2} \cdot \color{blue}{{im}^{2}} \]
    2. lift-*.f64N/A

      \[\leadsto 1 + \frac{-1}{2} \cdot {im}^{\color{blue}{2}} \]
    3. *-commutativeN/A

      \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
    4. lift-pow.f64N/A

      \[\leadsto 1 + {im}^{2} \cdot \frac{-1}{2} \]
    5. pow2N/A

      \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
    6. lift-*.f64N/A

      \[\leadsto 1 + \left(im \cdot im\right) \cdot \frac{-1}{2} \]
    7. +-commutativeN/A

      \[\leadsto \left(im \cdot im\right) \cdot \frac{-1}{2} + 1 \]
    8. lift-fma.f6428.7%

      \[\leadsto \mathsf{fma}\left(im \cdot im, -0.5, 1\right) \]
  9. Applied rewrites28.7%

    \[\leadsto \color{blue}{\mathsf{fma}\left(im \cdot im, -0.5, 1\right)} \]
  10. Add Preprocessing

Reproduce

?
herbie shell --seed 2025226 
(FPCore (re im)
  :name "math.exp on complex, real part"
  :precision binary64
  (* (exp re) (cos im)))